Appearance of a layer absorbing laser radiation near the surface of a metal target

Bergelson, Vitaly; Голуб, А. П.; Loseva, T. V.; Nemchinov, I. V.; Орлова, Т. И.; Popov, S. P.; Светцов, В. В.

doi:10.1070/qe1974v004n05abeh009299

Cited by 15 publications

(4 citation statements)

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“…They found that the laser spark characteristics were not very sensitive to the ambient conditions or the laser energy. This encouraged the quantitative use of laserinduced breakdown spectroscopy, which is becoming more common as a non-invasive measurement technique [10,16,17].…”

Section: Introductionmentioning

confidence: 99%

Laser-induced radical generation and evolution to a self-sustaining flame

Beduneau

Kawahara

Nakayama

et al. 2009

Combustion and Flame

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Section: Introductionmentioning

confidence: 99%

Laser-induced radical generation and evolution to a self-sustaining flame

Beduneau

Kawahara

Nakayama

et al. 2009

Combustion and Flame

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“…The following parameters were taken for C 2 molecular (in the units of cm -1 ) 39 (2) The values in the columns are for the ground, the first and the second electronic states, correspondingly. Except of C 2 spectral lines only CN lines additionally appeared in the spectra obtained for graphite target irradiation in the air.…”

Section: The Spectra Of Laser-produced Plasmamentioning

confidence: 99%

“…Density profiles at the moments t=100 (1), 200 (2), and 300 ns(3). Solid lines -EOS is an ideal gas, dashed lines -EOS is QEOS.…”

mentioning

confidence: 99%

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High-energy GARPUN KrF laser interaction with solid and thin-foil targets in ambient air

Зворыкин

Bakaev

Batani

et al. 2004

High-Power Laser Ablation V

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Hydrodynamic regimes of KrF laser interaction with solid and thin-film targets in atmospheric and reduced pressure air were investigated at high-energy GARPUN installation. These experiments were performed with 100-J, 100-ns laser pulses in planar focusing geometry and compared with numerical simulations with ATLANT code to verify the concept of laser-driven shock tube (LST), which could accelerate a gas to hypersonic velocity and produce strong shock waves (SW). Laser beam was focused by a prism raster optical system that provided very uniform intensity distribution at moderate laser intensities q ≤ 1 GW/cm 2 over a square spot of ~ 1-cm size. Dynamics of laser-produced plasma and SW in a surrounding gas were investigated by means of high-speed photo-chronograph and streak camera in combination with shadow or schlieren techniques, time and space resolved spectroscopy in a visible spectral range. Both experiments and simulations confirmed that target evaporation and blow-up of expanding plasma are the main mechanisms of UV laser-target interaction in a surrounding gas. Planar shock waves with velocities up to 7 km/s towards the laser beam were observed in a normal density air and up to 30 km/s in a rarefied air. Acceleration of thin CH films of 1 to 50-µm thickness was investigated both in a free-expansion and plasma-confined regimes with the highest achieved velocities up to 4 km/s. The SW damping law in a free space independently on laser intensity and air pressure could be approximated by a power law x ~ t n with a power indexes n 1 = 0.85 -0.95 at the initial stage and n 2 = 0.5 -0.6 later, when a distance of the SW front from a target became comparable with a size of the irradiated spot. Instability growth at contact interfaces between ablative plasma and accelerated film, as well as between plasma and compressed air were observed and compared for various initial irradiation non-uniformities. They were introduced by a grid, which was set in front of the film target.

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